XIX IMEKO World Congress Fundamental and Applied Metrology September 611, 2009, Lisbon, Portugal                   1 SAMEER- Centre for Electromagnetics, Chennai - 600113, India. 2 Institute of Electrical Measurement and Measurement Signal Processing, Graz University of Technology, Graz-8010, Austria, bgeorge@tugraz.at. 3 Dept. of Electrical Engineering, Indian Institute of Technology Madras, Chennai - 600036, India.  – A virtual instrumentation based scheme is developed for the characterization of magnetic materials. The principle used for measurement is derived from the comparison method of testing instrument transformers. A prototype has been developed by suitably modifying an instrument transformer test set. Characterization of magnetic materials at single frequency and multiple frequencies have been carried out. Typical test results obtained are presented in the paper. The developed instrument substantially reduces the testing time associated with magnetic characterization. : Instrument transformers, magnetic measurement, watt-loss measurement.   One of the largest users of magnetic materials in the form of laminations and toroidal cores is the electric power sector. Power transformers almost always use Si-steel laminations. Current transformers (CTs) are unique in that the magnetic structure is usually of a toroidal form. Depending on the application, CTs use high permeability Ni – Fe or Si – steel cores. Often, composite cores [1] are employed. Designers of CTs require the magnetic characteristics of core in the form of watt-loss and magnetizing ampere turns as a function of the flux density. Instruments with both sinusoidal B and H [2], [3] are available for performing such measurements. In the recent years, the advent of significant power electronic switching devices has meant that the voltage and current waveforms in the power network are not of a single frequency and contain significant harmonics. An instrument transformer test set for meeting this need has been designed [4]. It then becomes necessary to characterize the magnetic materials as a function of frequency. We develop a Virtual Instrumentation (VI) based scheme for this purpose. The new scheme uses a modified Instrument Transformer Test Set (ITTS) for the characterization of magnetic materials. The proposed method also shows a new application for the ITTS, with certain modifications, as an instrument for the characterization of magnetic materials. ! "" #      #   The Ratio Error (RE) and Phase Error (PE) in a CT are principally due to the excitation characteristic of the core and it is known [5] that + =  2 cos sin 100 % δ δ (1) min 3438 sin cos tan 2 1 ×  δ δ (2) where, m is the magnetizing component of exciting current, w is the watt-loss component of exciting current, δ is the secondary power factor angle and 2S is the secondary current. If the load is intentionally made to be unity power factor, equations (1) and (2) results in equations (3) and (4). 100 2 × =  (3) 3438 2  × = (4) This implies that the measurement of RE and PE in a transformer test bridge can enable a determination of and . If the dimensions of the core are available, magnetizing ampere turns ! " # = A/m (5) and watt loss ampere turns ! " # = A/m (6) can be evaluated, where ! is the mean length of the magnetic path and " is the number of secondary turns. If the range of secondary currents and burdens are chosen appropriately the instrument transformer test set can be used for characterizing the performance of the core material. The principal advantage of this method is that the result is in a form, which is directly useful for the CT design [1]. 682 ISBN 978-963-88410-0-1 © 2009 IMEKO